One-Particle Excitation of the Two-Dimensional Hubbard Model
arXiv:cond-mat/9702200 · doi:10.1143/JPSJ.66.529
Abstract
The real part of the self-energy of interacting two-dimensional electrons has been calculated in the t-matrix approximation. It is shown that the forward scattering results in an anomalous term leading to the vanishing renormalization factor of the one-particle Green function, which is a non-perturbative effect of the interaction U. The present result is a microscopic demonstration of the claim by Anderson based on the conventional many-body theory. The effect of the damping of the interacting electrons, which has been ignored in reaching above conclusion, has been briefly discussed.
7 pages, LaTeX, 1 figure, uses jpsj.sty, to be published in J. Phys. Soc. Jpn. 66 No. 3 (1997)
Cited by in corpus (5)
- Marginal Fermi liquid behavior from 2d Coulomb interaction
- Exact solutions for the periodic Anderson model in 2D: A Non-Fermi liquid state in normal phase
- Spectral Function of 2D Fermi Liquids
- New non-Fermi liquid type behavior given by a two-band system in normal phase
- Weak Coupling Phases of the Attractive Hubbard Model at the Van Hove Filling